We derive, using a finite-temperature path integral approach, the equation
for the phase boundary between the insulating and the superconducting phase
for quantum Josephson junctions arrays (JJA's) with offset charges and gen
eral capacitance matrices. We show that-within the mean field theory approx
imation-a reentrance in the phase boundary should appear, for systems with
a uniform distribution of offset charges, only when the capacitance matrix
is nondiagonal. For a model with nearest-neighbor capacitance matrix and un
iform offset charge q/2e=112, we find reentrant superconductivity even if t
he intergrain interaction is short ranged; for this model, we determine the
most relevant contributions to the equations for the phose boundary by exp
licitly constructing the charge distributions on the lattice corresponding
to the lowest-energy states which provide the leading contributions to the
partition function at low T-c.